centered_2nd_uniform
Stencil

Coefficients
| selector kind | axis | offset | coeff |
|---|---|---|---|
cartesian | $x | −1 | −1 / (2 dx) |
cartesian | $x | +1 | +1 / (2 dx) |
Combined as +. The result is the cell-centered approximation of the first
spatial derivative with a leading error term (dx² / 6) · u′′′(x).
Discrete operator
Applied to a cell-centered field \(u_i = u(x_i)\) on a uniform axis with spacing \(\Delta x\), the rule produces the discrete first-derivative operator
$$\left(\frac{\partial u}{\partial x}\right)_i \;\approx\; \frac{u_{i+1} - u_{i-1}}{2\,\Delta x}.$$Symmetric Taylor expansion of the two neighbors about \(x_i\),
$$u_{i\pm 1} \;=\; u_i \;\pm\; \Delta x\,u'_i \;+\; \tfrac{\Delta x^{2}}{2}\,u''_i \;\pm\; \tfrac{\Delta x^{3}}{6}\,u'''_i \;+\; \tfrac{\Delta x^{4}}{24}\,u^{(4)}_i \;\pm\; \cdots,$$cancels the even-order terms when subtracted, giving
$$\frac{u_{i+1} - u_{i-1}}{2\,\Delta x} \;=\; u'_i \;+\; \tfrac{\Delta x^{2}}{6}\,u'''_i \;+\; O(\Delta x^{4}).$$The scheme is therefore second-order accurate, with a purely dispersive
leading error \(\tfrac{\Delta x^{2}}{6}\,u'''(x)\) and no numerical
diffusion — contrast with upwind_1st,
whose one-sided stencil introduces an explicit diffusive
\((\Delta x / 2)\,u''(x)\) term.
Convergence

u(x) = sin(2πx)
on a periodic [0, 1] domain, sampled at cell centers. Empirical slope
matches the expected −2 reference line.The fixture under
discretizations/finite_difference/centered_2nd_uniform/fixtures/convergence/
sets expected_min_order = 1.9 to tolerate minor pre-asymptotic drift on
the 16 → 32 → 64 → 128 sequence.